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Titlebook: Experimental Techniques in Nuclear and Particle Physics; Stefaan Tavernier Textbook‘‘‘‘‘‘‘‘ 2010 Springer-Verlag Berlin Heidelberg 2010 Ne

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發(fā)表于 2025-3-27 00:57:43 | 只看該作者
32#
發(fā)表于 2025-3-27 02:51:41 | 只看該作者
Textbook‘‘‘‘‘‘‘‘ 2010hese constants in the equations, but that would probably be confusing for the engineering students.Physics students tend to be more interested in theoretical physics courses. However, physics is an experimental science and physics students should und- stand how experiments work, and be able to make
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發(fā)表于 2025-3-27 08:16:24 | 只看該作者
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發(fā)表于 2025-3-27 16:37:46 | 只看該作者
Handlungsfeld: Umgang mit Krankheit im Team,ery long lifetime occurring naturally; the most important of these is potassium-40. Several short-lived isotopes also occur naturally; these are either decay products of long-lived isotopes or are produced by cosmic rays. It is worth mentioning radon-222, which is an alpha emitter with a half-life o
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發(fā)表于 2025-3-27 21:15:50 | 只看該作者
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發(fā)表于 2025-3-28 01:45:11 | 只看該作者
Interactions of Particles in Matter,he subject, for references to the original literature, and for a derivation of many of the formula quoted in this chapter, see Ref. [4]. Reference [6, 9] of . are useful web resources containing extensive numerical data on the interactions of subatomic particles in matter.
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發(fā)表于 2025-3-28 06:00:34 | 只看該作者
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發(fā)表于 2025-3-28 10:03:21 | 只看該作者
Detectors Based on Ionisation in Gases,y first undergo an interaction. The charged particles produced in the interaction reveal that a neutral particle was present. Today there are three main methods for detecting charged subatomic particles that are important in nuclear science or in high-energy physics: detection based on gas ionisatio
40#
發(fā)表于 2025-3-28 11:25:04 | 只看該作者
Detectors Based on Ionisation in Semiconductor Materials,ased detectors, an advantage of semiconductors is that the amount of energy needed to produce one pair of free charge carriers is about a factor 10 less. Another important difference is that the density of a semiconductor is typically 1000 larger than the density of a gas. The primary charge signal
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